act on the leakage amplitude at the end of the gate. We show that this endpoint amplitude and the transient leakage exposure accumulated during the gate are two distinct control objectives that can be assigned to separate modules. The endpoint is a single sample of the drive spectrum, |Λ̃ (η)|2; the exposure is a band integral about η and governs leakage under dephasing, and the spectral-null condition Λ̃ (η)=0 constrains only the former. We realize this split in a path–endpoint separation pulse (PESP): a path-shaping pulse suppresses the exposure, and a two-tone endpoint-cancellation pulse cancels the residual amplitude. For a 10 ns RX(π/2) gate at η/2π=0.2 GHz, in numerical simulations the path-shaping pulse reduces the dephasing exposure by ∼21% relative to cosine DRAG and the independently simulated Lindblad excess leakage by ∼20%, consistent with Pϕexcess≃γϕTP¯dephA, whereas matched-budget endpoint-only and spectral-null controls leave it essentially unchanged. The residual endpoint floor splits exactly into a |2⟩ back-action and a |3⟩ cascade, which the two tones cancel one-to-one, driving the floor at the path-exposure knee from ∼7×10−7 to ∼3×10−8 without perturbing the path. By separating transient exposure from endpoint leakage, PESP turns leakage suppression in fast weakly anharmonic gates into a modular, interpretable control problem: dephasing-induced leakage and the coherent residual error are reduced by separate, individually verifiable modules.